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Methods that Circumventthe Second Law of Thermodynamics
Maxwell’s Demon: the Proell effectAtmospheric gravity separator: Chas. Steinmetz @ GE
Asymmetrical mechanical processes: Herb JohnsonAsymmetrical atomic processes: thermoelectrics, Daniel Sheehan at the
University of San DiegoAsymmetrical atomic processes: superconductivity, Peter Keefe at the University
of Detroit MercyAsymmetrical atomic processes: inverted populations of phase space, Steven
Smith’s magnetothermodynamics @ www.geocities.com/electrograviticsAsymmetrical atomic processes: infrared photovoltaics
Gibbs Free Energy changes: G = H – TS
Methods that Circumventthe Second Law of Thermodynamics
Maxwell’s Demon: the Proell effectAtmospheric gravity separator: Chas. Steinmetz @ GE
Asymmetrical mechanical processes: Herb JohnsonAsymmetrical atomic processes: thermoelectrics, Daniel Sheehan at the
University of San DiegoAsymmetrical atomic processes: superconductivity, Peter Keefe at the University
of Detroit MercyAsymmetrical atomic processes: inverted populations of phase space, Steven
Smith’s magnetothermodynamics @ www.geocities.com/electrograviticsAsymmetrical atomic processes: infrared photovoltaics
Gibbs Free Energy changes: G = H – TS
Methods that Circumventthe Second Law of Thermodynamics
Maxwell’s Demon: the Proell effectAtmospheric gravity separator: Chas. Steinmetz @ GE
Asymmetrical mechanical processes: Herb JohnsonAsymmetrical atomic processes: thermoelectrics, Daniel Sheehan at the
University of San DiegoAsymmetrical atomic processes: superconductivity, Peter Keefe at the University
of Detroit MercyAsymmetrical atomic processes: inverted populations of phase space, Steven
Smith’s magnetothermodynamics @ www.geocities.com/electrograviticsAsymmetrical atomic processes: infrared photovoltaics
Gibbs Free Energy changes: G = H – TS
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